Abstract
The anti-Stokes Raman laser is a perspective way to develop laser source to produce radiation with shorter wavelength. It is known that the effective anti-Stokes radiation can be obtained only under appropriate phase matching angle which is determined by the following phase matching condition Ka = 2KP - Ks. Here Kp> Ks and Ka are the pump, 1st Stokes and 1st anti-Stokes wave vectors correspondingly. In barium nitrate Raman crystal these angles were measured to be about 2° out of the crystal for 532 nm pump [1]
© 2000 IEEE
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